Probability of finding particle in shifted ground state

AegisAndAtrophy
Messages
4
Reaction score
0

Homework Statement


At t<0 a particle is in the ground state of the potential V(x)= \frac{1}{2} mw^2x^2. At t=0 the potential is suddenly displaced by an amount x0 to V(x)= \frac{1}{2} mw^2(x-x_0)^2 .

a) What is the probability of the particle being in the ground state; the first excited state?
b) At t=\frac{2pi}{w} write the wave function

Homework Equations

The Attempt at a Solution


I think that the wave function should be Ψ_0(x,0)= (\frac{mw}{πh})^\frac{1}{4} e^ \frac{-mw(x-x_0)^2}{2h}
I'm not sure what I should do though in order to find the probability in the ground state.
For the first excited energy I know I need to use the raising operator in order to get the wave function, which would give me (\frac{mw}{h})^\frac{1}{2} times Ψ_0 but again I'm unsure how to find the probability.
 
Physics news on Phys.org
Express the original state in terms of the new ones.
 
I'm not exactly sure what you mean in order to go about doing that.
 
The particle still has the same wavefunction after the potential has been changed.
However, that no longer corresponds to an energy eigenstate.
Expand the original wavefunction as a linear sum of the new energy eigenstates.
What do the coefficients of the expansion represent?
 
So I should expand Ψ =∑CnΨn where |Cn|^2 is the probability of the new energy eigenstate?
 
Does the change in time from t<0 to t=0 not affect it in any way?
 
The effect is in the possible outcome of future measurements.
 
AegisAndAtrophy said:

Homework Statement


At t<0 a particle is in the ground state of the potential V(x)= \frac{1}{2} mw^2x^2. At t=0 the potential is suddenly displaced by an amount x0 to V(x)= \frac{1}{2} mw^2(x-x_0)^2 .

a) What is the probability of the particle being in the ground state; the first excited state?
b) At t=\frac{2pi}{w} write the wave function

Homework Equations

The Attempt at a Solution


I think that the wave function should be Ψ_0(x,0)= (\frac{mw}{πh})^\frac{1}{4} e^{-\frac{mw(x-x_0)^2}{2h}}
This is the ground state of the system after the potential is displaced. It's not the state of the particle at ##t=0##, which is still in the state
$$\Psi(x,0) = \left(\frac{m\omega}{πh}\right)^\frac{1}{4} e^{-\frac{m\omega x^2}{2h}}.$$ By the way, the frequency is denoted by the Greek letter ##\omega##, not ##w##.

I'm not sure what I should do though in order to find the probability in the ground state.
For the first excited energy I know I need to use the raising operator in order to get the wave function, which would give me (\frac{mw}{h})^\frac{1}{2} times Ψ_0 but again I'm unsure how to find the probability.
Look up the definition of the probability amplitude. This is a basic definition you need to know.
 
Back
Top